Internal Multiphase Targets Non destructive electromagnetic detectors Astrophysics in Storage Rings Non destructive electromagnetic detectors Laser spectroscopy Internal Multiphase Targets

rate for Z=120 is predicted for the most mass asymmetric projectile/target combination 54Cr + 248Cm. However, at SHIP no radioactive targets could be used up to now. Therefore, we took the reaction 64Ni + [...] identify Z=114 as shell closure, we investigated as further candidate Z=120. Three different projectile-target combinations lead to the same compound nucleus 302120: 64Ni + 238U, 58Fe + 244Pu and 54Cr + 248Cm [...] chain of element 120 was found. With the total number of 2.6×1019 projectiles which impinged the target, it converts to an upper cross-section limit of 90 fb. From this result we can deduce, that the stability

Experiments Information for GSI-/FAIR-Guests Detectors Development Electron Spectrometer Electron Target / Cooler High Energy Single Pass Experiment s Laser Cooling Laser Spectroscop y Photon and X-Ray [...] Spectrometer Photon Detektor Development Ring Physics and Performance Slow Ion/Surface Experiments Target Development

Abmessungen der PPT98-Targets Beryllium I, cylindrical target weight m 1563,360 mg length h 10,812 mm diameter Ø 9,981 mm area A 0,782 cm² aereal weight m/A 1998,117 mg/cm² density r 1,848 g/cm³

U28+ and Xe18+ Ions (pdf-File) Projectile Electron Losses in the Collision with Neutral Targets (pdf-File) Novel Target Developments for FAIR (pdf-File) A Reaction Microscope with Toroidal Sectors (pdf-File) [...] Si(Li) detector System (pdf-File) Improvements of the cryogenic target beam source at the ESR (pdf-File) A pulsed supersonic gas jet target for HITRAP (pdf-File) Laser cooling of relativistic ion beams [...] spectrometer for studies with helium-like argon (pdf-File) The New Gas Jet Target for Experiments at HITRAP (pdf-File) The Gas Jet Target for Experiments at HITRAP (pdf-File) The High Voltage Electron Beam Ion

Special Installations The special installation of the Super-FRS are mainly the production target and beam catchers for high intensity beams. Because of activation it also involves the iron shielding of [...] degraders and parts of the gas stopping cell also belong to the special installations. Super-FRS target area (front part of shielding removed).

section of the coupling beamline from the synchrotrons to the Super-FRS target, FPF0. The Super-FRS itself starts from that production target. The first fragment-selection stage is the Pre-Separator . Then come [...] three branches of the Super-FRS, as well as simulations of, e.g., the beam spot size at detector and target locations for future NUSTAR RIB experiments. The principal ion-optical programs used are GICOSY

can be focused to a spot of less than 300 µm (FWHM) at the target. Assuming a solid metallic target, the specific energy deposition in the target material is from a few kJ/g to ~ 50 kJ/g. This correspond [...] with heavy-ion excitation) nuclear and particle physics (design and tests of high-load production targets and beam dumps, diamond detector R&D) accelerator technology (diagnostics of powerful ion beams,

Illustration of selected nuclear fragmentation reaction channels by 4He ions colliding with 12C target nuclei [figure from F Horst [1]] Schematic (left) and photo (right) of the experimental setup used [...] used at HIT to measure nuclear reaction cross sections for 4He ions impinging on different targets [figure from F Horst [1]] References: [1] F. Horst, Measurement of Nuclear Reaction Cross Sections for [...] F. Horst et al., Measurement of 4He charge- and mass-changing cross sections on H, C, O, and Si targets in the energy range 70-220 MeV/u for radiation transport calculations in ion-beam therapy, Phys.

are accelerated over a few μm along the target normal direction. After the acceleration process is over and the target is disrupted (~ns), the ions leave the target in a quasi-neutral cloud together with [...] High-Energy Laser for Heavy Ion EXperiments (PHELIX) hits a solid target (E < 25 J, τ = 500 fs, I > 10 19 J/cm 2 ) and drives the TNSA (Target Normal Sheath Acceleration) mechanism. A selected part of the [...] critical surface and accelerates hot electrons into the target material (b). The electrons are transported under a divergence angle through the target, leave the rear side and form a dense electron sheath